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where Vmin , and Vmax are the curvatures at the potential maximum and minimum and V is the height of the barrier. Experimentally the first passage time and its dependence on the feedback strength, or on the phase of the feedback, can be determined by monitoring the power of the laser with a fast oscilloscope. Since the two modes have different powers, and of course different frequencies, the modes can be identified by the intensity levels. Since noise is an important ingredient, and strongly affects the first passage time, it is of considerable importance to drive the laser with an ultralow-noise current source and for it to be temperature stabilized [32]. Figure 4.7 shows the experimentally obtained evolution of the oscillation frequency of a 1.3 m DFB laser and the corresponding potential wells obtained from Equation (4.13) for three different values of the phase. The feedback strength is 45 7 dB and for the lower 0. The trace shows mode hopping between trace the relative phase is set to 0 + tan 1 three modes 250 MHz apart corresponding to the external cavity round-trip frequency. The absolute minimum of the potential is at the solitary laser frequency, and the laser infrequently can jump to either of the two wells adjacent to the main one. The top trace is obtained for where the solitary laser frequency lies exactly between a relative phase 0 + tan 1 the minima. Here the laser can visit the two wells with equal frequency. The middle trace 1 4 and shows the intermediate situation. The experimental is taken for 0 + tan 1 data in Figure 4.8 show the frequency evolution as a function of time for different feedback . levels with the feedback phase adjusted for maximum hopping rate to 0 + tan 1 java ean 13 EAN - 13 Java Control- EAN - 13 barcode generator for Java with Java ...
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